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dc.contributor.authorÖzbay, Ekmelen_US
dc.contributor.authorTemelkuran, B.en_US
dc.contributor.authorSigalas, M.en_US
dc.contributor.authorTuttle, G.en_US
dc.contributor.authorSoukoulis, C. M.en_US
dc.contributor.authorHo, K. M.en_US
dc.date.accessioned2015-07-28T11:56:10Z
dc.date.available2015-07-28T11:56:10Z
dc.date.issued1996-12-16en_US
dc.identifier.issn0003-6951
dc.identifier.urihttp://hdl.handle.net/11693/10882
dc.description.abstractWe have investigated metallic photonic crystals built around a layer‐by‐layer geometry. Two different crystal structures (face‐centered‐tetragonal and tetragonal) were built and their properties were compared. We obtained rejection rates of 7–8 dB per layer from both metallic crystals. Defect modes created by removing rods resulted in high peak transmission (80%), and high quality factors (1740). Our measurements were in good agreement with theoretical simulations.en_US
dc.language.isoEnglishen_US
dc.source.titleApplied Physics Lettersen_US
dc.relation.isversionofhttp://dx.doi.org/10.1063/1.117002en_US
dc.subjectBand-gap Crystalsen_US
dc.subjectCavityen_US
dc.subjectLaseren_US
dc.titleDefect structures in metallic photonic crystalsen_US
dc.typeArticleen_US
dc.departmentDepartment of Physicsen_US
dc.departmentDepartment of Electrical and Electronics Engineeringen_US
dc.departmentInstitute of Materials Science and Nanotechnology (UNAM)en_US
dc.citation.spage3797en_US
dc.citation.epage3799en_US
dc.citation.volumeNumber69en_US
dc.citation.issueNumber25en_US
dc.identifier.doi10.1063/1.117002en_US
dc.publisherA I P Publishing LLCen_US
dc.contributor.bilkentauthorÖzbay, Ekmel
dc.identifier.eissn1077-3118


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